{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:PUUDP2Q4MBTSBAICYVYEVN4ER3","short_pith_number":"pith:PUUDP2Q4","canonical_record":{"source":{"id":"1107.4078","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-20T19:21:49Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"d081ae4d2ca56afa182209ccae3fa518a691f80f31c320ce544c08344145498c","abstract_canon_sha256":"90d4b3070ce09b5c24df52a8cd690aa55c5c8a9a7bdb106c8458ab3fca5cdfea"},"schema_version":"1.0"},"canonical_sha256":"7d2837ea1c6067208102c5704ab7848ed4d6d985915ffbf526a4ac44442ec520","source":{"kind":"arxiv","id":"1107.4078","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1107.4078","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"arxiv_version","alias_value":"1107.4078v2","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.4078","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"pith_short_12","alias_value":"PUUDP2Q4MBTS","created_at":"2026-05-18T12:26:39Z"},{"alias_kind":"pith_short_16","alias_value":"PUUDP2Q4MBTSBAIC","created_at":"2026-05-18T12:26:39Z"},{"alias_kind":"pith_short_8","alias_value":"PUUDP2Q4","created_at":"2026-05-18T12:26:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:PUUDP2Q4MBTSBAICYVYEVN4ER3","target":"record","payload":{"canonical_record":{"source":{"id":"1107.4078","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-20T19:21:49Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"d081ae4d2ca56afa182209ccae3fa518a691f80f31c320ce544c08344145498c","abstract_canon_sha256":"90d4b3070ce09b5c24df52a8cd690aa55c5c8a9a7bdb106c8458ab3fca5cdfea"},"schema_version":"1.0"},"canonical_sha256":"7d2837ea1c6067208102c5704ab7848ed4d6d985915ffbf526a4ac44442ec520","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:00:15.795371Z","signature_b64":"zQC6e5pnQ0rf78dePKK/cqeu8MW6PSyQy644qExW2EY116OnzhS0qmSn6ig669bLrznNchJvJSQviQxW6PGgDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d2837ea1c6067208102c5704ab7848ed4d6d985915ffbf526a4ac44442ec520","last_reissued_at":"2026-05-18T04:00:15.794613Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:00:15.794613Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1107.4078","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:00:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cWxrgvi075LbiY2l3rnGIut/YFC52RqCeJ++vmGSngmWCHb0T21NRhGEircibemA7tEyHEZXBv94/XOplteHDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T04:49:06.985754Z"},"content_sha256":"100be699490a49162c31aaf9160f3ed72d7d9490401efd61e5f5af73c5de144c","schema_version":"1.0","event_id":"sha256:100be699490a49162c31aaf9160f3ed72d7d9490401efd61e5f5af73c5de144c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:PUUDP2Q4MBTSBAICYVYEVN4ER3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The curvaton scenario in the MSSM and predictions for non-Gaussianity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Anupam Mazumdar, Seshadri Nadathur","submitted_at":"2011-07-20T19:21:49Z","abstract_excerpt":"We provide a model in which both the inflaton and the curvaton are obtained from within the minimal supersymmetric Standard Model, with known gauge and Yukawa interactions. Since now both the inflaton and curvaton fields are successfully embedded within the same sector, their decay products thermalize very quickly before the electroweak scale. This results in two important features of the model: firstly, there will be no residual isocurvature perturbations, and secondly, observable non-Gaussianities can be generated with the non-Gaussianity parameter $f_\\mathrm{NL}\\sim {\\cal O}(5-1000)$ being "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.4078","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:00:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zpdgz2LBU0JYI8AxAkxYvqavxCAEAJ8iE0vLFc9EFFUlvLql3PDtO2i9pEQFCp6U0GJYKHKbf7WSQ7UoZn57AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T04:49:06.986443Z"},"content_sha256":"09aa9e103c44849203debc7b63196a9c3cddc63c13a9f713a9617e7f1c94a6e0","schema_version":"1.0","event_id":"sha256:09aa9e103c44849203debc7b63196a9c3cddc63c13a9f713a9617e7f1c94a6e0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3/bundle.json","state_url":"https://pith.science/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-10T04:49:06Z","links":{"resolver":"https://pith.science/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3","bundle":"https://pith.science/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3/bundle.json","state":"https://pith.science/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PUUDP2Q4MBTSBAICYVYEVN4ER3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:PUUDP2Q4MBTSBAICYVYEVN4ER3","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"90d4b3070ce09b5c24df52a8cd690aa55c5c8a9a7bdb106c8458ab3fca5cdfea","cross_cats_sorted":["astro-ph.CO"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-20T19:21:49Z","title_canon_sha256":"d081ae4d2ca56afa182209ccae3fa518a691f80f31c320ce544c08344145498c"},"schema_version":"1.0","source":{"id":"1107.4078","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1107.4078","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"arxiv_version","alias_value":"1107.4078v2","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.4078","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"pith_short_12","alias_value":"PUUDP2Q4MBTS","created_at":"2026-05-18T12:26:39Z"},{"alias_kind":"pith_short_16","alias_value":"PUUDP2Q4MBTSBAIC","created_at":"2026-05-18T12:26:39Z"},{"alias_kind":"pith_short_8","alias_value":"PUUDP2Q4","created_at":"2026-05-18T12:26:39Z"}],"graph_snapshots":[{"event_id":"sha256:09aa9e103c44849203debc7b63196a9c3cddc63c13a9f713a9617e7f1c94a6e0","target":"graph","created_at":"2026-05-18T04:00:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We provide a model in which both the inflaton and the curvaton are obtained from within the minimal supersymmetric Standard Model, with known gauge and Yukawa interactions. Since now both the inflaton and curvaton fields are successfully embedded within the same sector, their decay products thermalize very quickly before the electroweak scale. This results in two important features of the model: firstly, there will be no residual isocurvature perturbations, and secondly, observable non-Gaussianities can be generated with the non-Gaussianity parameter $f_\\mathrm{NL}\\sim {\\cal O}(5-1000)$ being ","authors_text":"Anupam Mazumdar, Seshadri Nadathur","cross_cats":["astro-ph.CO"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-20T19:21:49Z","title":"The curvaton scenario in the MSSM and predictions for non-Gaussianity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.4078","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:100be699490a49162c31aaf9160f3ed72d7d9490401efd61e5f5af73c5de144c","target":"record","created_at":"2026-05-18T04:00:15Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"90d4b3070ce09b5c24df52a8cd690aa55c5c8a9a7bdb106c8458ab3fca5cdfea","cross_cats_sorted":["astro-ph.CO"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-20T19:21:49Z","title_canon_sha256":"d081ae4d2ca56afa182209ccae3fa518a691f80f31c320ce544c08344145498c"},"schema_version":"1.0","source":{"id":"1107.4078","kind":"arxiv","version":2}},"canonical_sha256":"7d2837ea1c6067208102c5704ab7848ed4d6d985915ffbf526a4ac44442ec520","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7d2837ea1c6067208102c5704ab7848ed4d6d985915ffbf526a4ac44442ec520","first_computed_at":"2026-05-18T04:00:15.794613Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:00:15.794613Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zQC6e5pnQ0rf78dePKK/cqeu8MW6PSyQy644qExW2EY116OnzhS0qmSn6ig669bLrznNchJvJSQviQxW6PGgDw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:00:15.795371Z","signed_message":"canonical_sha256_bytes"},"source_id":"1107.4078","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:100be699490a49162c31aaf9160f3ed72d7d9490401efd61e5f5af73c5de144c","sha256:09aa9e103c44849203debc7b63196a9c3cddc63c13a9f713a9617e7f1c94a6e0"],"state_sha256":"4f627d4a29c7c932baaf4f95e357144482c655a40bfbcf60506d3f0d0dfe63ef"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0l0JK1na1rVl6TDaTytQZ9WHlvzspCvWTNnieiZEclRiHhnjyaeA9BUOcBOEQyV+oTAOercWLEwKy4qAi0QFBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T04:49:06.990050Z","bundle_sha256":"46ed38c69091cf2a0debc871d2179bd57034785413e6516b5132f8d6246b121b"}}